论文标题
Asassn-18am/sn 2018GK:庞大的祖细胞中的过多的IIB超新星
ASASSN-18am/SN 2018gk : An overluminous Type IIb supernova from a massive progenitor
论文作者
论文摘要
Asassn-18am/sn 2018GK是稀有的富含氢的超新星(SNE)的新发现的成员,峰值绝对幅度为$ m_v \ -20 $ mag,位于正常的核心collapse sne和超浮肿的SNE之间。这些SNE没有显示出与偶色材料(CSM)相互作用的突出光谱特征,其动力机制是有争议的。对于II型SN,Asassn-18AM的下降速度极快,光电相的下降率为$ \ sim6.0〜 \ rm mag〜(100 d)^{ - 1} $。由于HI的弱化和HEI在其后期的外观,Asassn-18am在光谱上是IIB型SN,带有部分剥离的信封。但是,其光度和光谱进化显示与典型的SNE IIB有显着差异。使用辐射扩散模型,我们发现光曲线需要一个高的合成$ \ rm ^{56} ni $ $ mass $ m _ {\ rm ni} \ sim0.4〜m_ \ odot $和带有高动能$ e _ e _ _ {\ rmkin kin} $ erg的$ e _ m_ \ odot $和ejecta $ erg引入磁盘中央引擎仍然需要$ M _ {\ rm ni} \ sim0.3〜m_ \ odot $和$ e _ {\ rm kin} = 3 \ times10^{51} $ erg。高$ \ rm ^{56} ni $质量与其光谱中的强铁组卵形线一致,它们也类似于几个具有高$ \ rm ^{56} ni $产量的sne ic-bl。最早的频谱显示了“闪存电离”功能,我们从中估算出$ \ dot {m} \左右2 \ times10^{ - 4}〜\ rm m_ \ odot〜yr^yr^{ - 1} $的质量损失率。这种风密度太低,无法通过射流CSM相互作用为发光光曲线供电。对于$H_α$,我们的估计膨胀速度高达$ 17,000 $ km/s,与其他SNE II相比,这非常高。我们估计使用使用[oi]亮度的氧气核心质量为$ 1.8-3.4 $ $ $ m_ \ odot $,它是通过nebular-phase spectrum测量的,这意味着祖先的祖先为零时代的主序质量为$ 19-26 $ $ $ $ $ $ m_ \ odot $。
ASASSN-18am/SN 2018gk is a newly discovered member of the rare group of luminous, hydrogen-rich supernovae (SNe) with a peak absolute magnitude of $M_V \approx -20$ mag that is in between normal core-collapse SNe and superluminous SNe. These SNe show no prominent spectroscopic signatures of ejecta interacting with circumstellar material (CSM), and their powering mechanism is debated. ASASSN-18am declines extremely rapidly for a Type II SN, with a photospheric-phase decline rate of $\sim6.0~\rm mag~(100 d)^{-1}$. Owing to the weakening of HI and the appearance of HeI in its later phases, ASASSN-18am is spectroscopically a Type IIb SN with a partially stripped envelope. However, its photometric and spectroscopic evolution show significant differences from typical SNe IIb. Using a radiative diffusion model, we find that the light curve requires a high synthesised $\rm ^{56}Ni$ mass $M_{\rm Ni} \sim0.4~M_\odot$ and ejecta with high kinetic energy $E_{\rm kin} = (7-10) \times10^{51} $ erg. Introducing a magnetar central engine still requires $M_{\rm Ni} \sim0.3~M_\odot$ and $E_{\rm kin}= 3\times10^{51} $ erg. The high $\rm ^{56}Ni$ mass is consistent with strong iron-group nebular lines in its spectra, which are also similar to several SNe Ic-BL with high $\rm ^{56}Ni$ yields. The earliest spectrum shows "flash ionisation" features, from which we estimate a mass-loss rate of $ \dot{M}\approx 2\times10^{-4}~\rm M_\odot~yr^{-1} $. This wind density is too low to power the luminous light curve by ejecta-CSM interaction. We measure expansion velocities as high as $ 17,000 $ km/s for $H_α$, which is remarkably high compared to other SNe II. We estimate an oxygen core mass of $1.8-3.4$ $M_\odot$ using the [OI] luminosity measured from a nebular-phase spectrum, implying a progenitor with a zero-age main sequence mass of $19-26$ $M_\odot$.